How Will JDEM Learn About Dark Energy?
|Before (right) and after (left) image of Supernova 1987A|
At the same time, deep within the star, its core compresses, getting denser and denser. The immense pressure squeezes it into a ball just a few thousand miles across, roughly the size of the Earth. In a normal star, the heat generated in the core supports it against its own gravity. In the compressed core, the support is due to a weird quantum mechanical effect called "degeneracy". The electrons strongly resist being forced together, and repel each other quite strongly. This repulsion, distinct from the electric repulsion between charged particles and much stronger, is what keeps the core from collapsing any further. Since the outer layers of the star are gone, blown away in the stellar wind, the core is exposed to space. It's very hot, glowing white, but it's small and dense. We call it a white dwarf.
Type 1a SupernovaeFor the Sun, the story will end here. In a few billion years, it will become a white dwarf after shedding its outer layers.
But if the original star was closely orbiting another star, things could be different. This is called a binary system. Eventually, the companion star will also run out of hydrogen, and its outer layers will expand away. As these layers expand, some of the material from the star can be drawn onto the white dwarf, creating a thin layer on its surface. If the flow is really weak, the immense heat of the dwarf can prevent this from happening, but if the flow is very heavy, the matter piles up quickly, gets compressed by the huge gravity of the white dwarf, and undergoes explosive thermonuclear fusion. Bang! The star experiences a pretty big explosion on its surface, but it survives. Eventually matter begins to accumulate again, and the process repeats itself. This is called a recurrent nova.
| Artist conception of binary with a whte dwarf, prior
to exploding, courtesy Don Dixon
This is a supernova. Technically, it's called a Type Ia supernova (a massive star exploding is a Type II). The explosion energy seen in visible light is roughly 1044 Joules, as much energy as the Sun puts out over its entire lifetime, all in a few seconds.
Standard Candles in the Dark
One of the most interesting aspects of this type of supernova is that the white dwarf needs to have a very specific mass to explode-1.44 solar masses. This means that the explosion energy of a Type Ia is always roughly the same, no matter where we see it. This makes them incredibly useful to astronomers. Why? Because if you know how bright an object should be, and measure how bright it appears, you can determine its distance. Just like a distant car has faint headlights, but up close they are blindingly bright, a Type Ia supernova gets fainter with distance in a well-determined way.
|Standard candles are objects which are the same absolute brightness, and their distance can be determined by measuring their apparent brightness.|
In 1998, two teams of astronomers exploited this fact to compare the apparent brightnesses of many Type Ia supernovae that were very far away-billions of light years distant. They compared this to what was expected from the distances as measured by the redshifts and were shocked to discover that the supernovae were all fainter than expected. They went through an exhaustive checklist to make sure their results weren't influenced by other factors, like dust in the supernova, or differences in chemistry of very distant stars. But it all checked out, and they were left with an incredible conclusion: the supernovae were actually farther away than their redshift distances naively indicated.
If the supernovae are farther away than expected, then the expansion of the Universe must be accelerating! Most astronomers assumed it would be slowing down because the gravity of all the combined objects in the Universe would be hitting the cosmic brakes. Instead, the opposite was happening. This was perhaps the biggest scientific shock of the late 20th Century.
|Before (left) and after (right) images of a supernova exploding in a distant galaxy.|
Using the tools available (such as giant ground-based telescopes and the orbiting Hubble Space Telescope) astronomers can see Type Ia supernovae out to a distance of about 7 billion light years-a redshift of 1. And even then it's very hard, since you never know when or where one will pop off. But to really see the cosmic acceleration well, and to measure it accurately, astronomers need to see farther out.
This is where JDEM comes in. With its superior viewing position of deep space, excellent optics, and wide-field detector, it can detect supernovae at redshifts of 1.7, almost 10 billion light years distant. This is far enough away that the signature of the acceleration will be easy to spot. The wide field allows astronomers to watch large numbers of distant galaxies for the tell-tale signs of an exploding star, to distinguish between the two types of supernovae, and to get excellent data on the redshifts of the events. Altogether, this makes JDEM the perfect tool to measure these titanic explosions at cosmic distances.
Weak LensingOne of Albert Einstein's greatest contributions to science was the idea that space-time is not just a static stage in which objects move, but a dynamic player. Einstein realized that the force of gravity is due to the interaction of matter and space-time. Space-time is bent, warped, distorted where there is matter. The more matter there is within a certain amount of space, the more the distortion. Objects travel along curved paths through this warped space-time.
| In this Hubble image, a cluster of galaxies
has strongly distorted the images of more distant
galaxies. The distant galaxies have been warped
into long, thin arcs due to gravitational lensing.
Imagine a large square sheet of rubber being held at its corners by four people. It will be flat, but if you put a heavy object in the center, it will create a dimple in the sheet. If you roll a marble across the sheet, its path will curve around the heavier object. This is very much like how matter distorts space, and how objects behave under that influence-except space isn't flat like a sheet, it has three dimensions. This makes it difficult to picture, but the sheet makes a good analogy.
But since space itself is bent by matter, Einstein realized that any light traveling through that region of bent space will have its path changed too. It takes a pretty hefty mass to make a measurable change in the path of a beam of light, but nature has provided us with galaxies massive enough to do the trick.
Imagine a very distant galaxy, with another galaxy or a cluster of galaxies between us and it. The light from the more distant galaxy will get bent around the intervening object, distorting how we see its shape. The galaxy in the middle acts like a lens, and in fact it's called a "gravitational lens". Many such examples have been found in astronomical images. In some cases the lensing is very strong, and you can see arcs and multiple images of objects. In other cases the lensing is weaker, and the distant object's shape is only subtly distorted. In most cases the actual galaxy doing the lensing is invisible, but we can infer its existence from the distortions it causes.
Through a Lens, Weakly
|Imagine this grid of colors represents distant galaxies, with no matter between them and us...||... then, if there are galaxies between us, this picture represents how that grid gets distorted by the gravity of those galaxies. That's lensing.|
These weak lenses play a big role in cosmology. By mapping out the distortion of distant objects, we can build up a map of matter in the Universe that is causing the lensing. The amount and shape of the distortion tells astronomers quite a bit about the properties of that matter, too, including its distance.
Why is this important? Distant supernovae allow JDEM to measure the expansion history of the Universe, but cannot tell us whether accelerated expansion is due to dark energy (either a cosmological constant or quintessence) or a property of gravity we don't yet understand. Weak lensing, however, is very sensitive to both the distribution of matter and the details of gravity. Distortions from this weak lensing effect provide a map of the matter in the Universe not just across the sky, but also provide a distance as well - and at these distances, looking across space is the same as looking back in time. The farther away the object is, the longer it took for its light to get here, and thus the younger the Universe was when the light left it. Weak lensing gives astronomers a 3D map of the matter in Universe.
This is critical! Because dark energy pulls the Universe apart, the ability of matter to clump together to form galaxies and clusters changes as dark energy changes. By looking at how matter clumps now versus how it clumped, say, 5 billion years ago, astronomers can determine if the amount of dark energy in the Universe is constant or increases with time.
Baryon Acoustic Oscillations
Baryon acoustic oscillation (BAO) is a fancy name for the way galaxies in our universe tend to bunch up roughly every 480 million light years. This density variation at regular intervals is used as a natural measuring stick, or a "standard ruler" for measuring how the universe has expanded since early in its history, and thus the properties of dark energy.
Origin of BAO
What caused these density variations? In the beginning, the Big Bang universe was hot, dense, and smooth. However, during first fraction of a second of the cosmos when the cosmos was undergoing rapid expansion, called inflation, imbalances to the otherwise smooth universe is thought to have been introduced by quantum fluctuations. These pressure imbalances in the cosmos then caused the early cosmos in plasma state to oscillate like sound waves. About 380,000 years after the Big Bang, the universe cooled enough to allow protons and electrons to form hydrogen, and the distance a sound wave could have traveled in this time defines a standard length. With the subsequent thousandfold expansion of the universe, this spherical sound wave has now stretched to a radius of 480 million light-years which can be used as a standard ruler to measure the history of the expansion of the universe.
Temperature fluctuations in the cosmic microwave background are directly related to the density variations of galaxies as observed today.
How does the BAO method differ from the Supernovae method? The BAO method uses regular galaxy density variations as standard rulers - measurement of apparent size. In contrast, the Supernova method uses Type Ia supernovae as standard candles - measurement of apparent brightness.
With the supernovae method, redshift of supernovae are compared to the distances calculated by using the supernovae apparent brightness.
|Standard candle or apparent brightness-object becomes fainter by the square of its distance.|
With the BAO method, the distance for redshift measurements is calculated by using the apparent size of the comoving separation (distance that adjusts for the expansion of the universe) of 480 million light-years.
|Standard ruler or apparent size- distance to the object calculated by the apparent size of the object.|
Observations of supernovae, weak lensing, and baron acoustic oscillations together can provide the key to distinguishing between the three models of dark energy. This is just what JDEM is designed to do. It will take the measure of both supernovae, weak lensing, and baryon acoustic oscillations, and by the careful combined analysis of the three, the nature of dark energy may be unlocked.